Energy quantisation and time parameterisationFaraggi, Alon E.;Matone, Marco
doi: 10.1140/epjc/s10052-013-2694-1pmid: N/A
Abstract We show that if space is compact, then trajectories cannot be defined in the framework of the quantum Hamilton–Jacobi (HJ) equation. The starting point is the simple observation that when the energy is quantised it is not possible to make variations with respect to the energy, and the time parameterisation \(t-t_0=\partial _E{\mathcal {S}}_0\), implied by Jacobi’s theorem, which leads to the group velocity, is ill defined. It should be stressed that this follows directly from the quantum HJ equation without any axiomatic assumption concerning the standard formulation of quantum mechanics. This provides a stringent connection between the quantum HJ equation and the Copenhagen interpretation. Together with tunnelling and the energy quantisation theorem for confining potentials, formulated in the framework of quantum HJ equation, it leads to the main features of the axioms of quantum mechanics from a unique geometrical principle. Similar to the case of the classical HJ equation, this fixes its quantum analog by requiring that there exist point transformations, rather than canonical ones, leading to the trivial hamiltonian. This is equivalent to a basic cocycle condition on the states. Such a cocycle condition can be implemented on compact spaces, so that continuous energy spectra are allowed only as a limiting case. Remarkably, a compact space would also imply that the Dirac and von Neumann formulations of quantum mechanics essentially coincide. We suggest that there is a definition of time parameterisation leading to trajectories in the context of the quantum HJ equation having the probabilistic interpretation of the Copenhagen School.
Net baryon number probability distribution near the chiral phase transitionMorita, Kenji;Skokov, Vladimir;Friman, Bengt;Redlich, Krzysztof
doi: 10.1140/epjc/s10052-013-2706-1pmid: N/A
Abstract We discuss the properties of the net baryon number probability distribution near the chiral phase transition to explore the effect of critical fluctuations. Our studies are performed within Landau theory, where the coefficients of the polynomial potential are parametrized, so as to reproduce the mean-field (MF), the \(Z(2)\), and the \(O(4)\) scaling behaviors of the cumulants of the net baryon number. We show that in the critical region the structure of the probability distribution changes, depending on the values of the critical exponents. In the MF approach, as well as in the \(Z(2)\) universality class, the contribution of the singular part of the thermodynamic potential tends to broaden the distribution. By contrast, in the model with \(O(4)\) scaling, the contribution of the singular part results in a narrower net baryon number probability distribution with a wide tail.
Many-body problem in Kaluza–Klein models with toroidal compactificationChopovsky, Alexey;Eingorn, Maxim;Zhuk, Alexander
doi: 10.1140/epjc/s10052-013-2700-7pmid: N/A
Abstract In this paper, we consider a system of gravitating bodies in Kaluza–Klein models with toroidal compactification of the extra dimensions. To simulate the astrophysical objects (e.g., our Sun and pulsars) with energy density much greater than the pressure, we assume that these bodies are pressureless in the external space, i.e., the space we inhabit. At the same time, they may have nonzero parameters \(\omega _{({\bar{\alpha }} -3)} \, ({\bar{\alpha }} =4,\ldots , D)\) in the equations of state in the extra dimensions. We construct the Lagrange function of this many-body system for any value of \(\Sigma =\sum _{{\bar{\alpha }}} \omega _{({\bar{\alpha }} -3)}\). Moreover, the gravitational tests (PPN parameters, perihelion and periastron advances) require a negligible deviation from the latent soliton value \(\Sigma =-(D-3)/2\). However, the presence of pressure/tension in the internal space results necessarily in the smearing of the gravitating masses over the internal space and in the absence of KK modes. This looks very unnatural from the point of view of quantum physics.
Canonical approach to the closed string non-commutativityDavidović, Lj.;Nikolić, B.;Sazdović, B.
doi: 10.1140/epjc/s10052-014-2734-5pmid: N/A
Abstract We consider the closed string moving in a weakly curved background and its totally T-dualized background. Using T-duality transformation laws, we find the structure of the Poisson brackets in the T-dual space corresponding to the fundamental Poisson brackets in the original theory. From this structure we see that the commutative original theory is equivalent to the non-commutative T-dual theory, whose Poisson brackets are proportional to the background fluxes times winding and momentum numbers. The non-commutative theory of the present article is more nongeometrical than T-folds and in the case of three space-time dimensions corresponds to the nongeometric space-time with \(R\)-flux.
Shaping the distribution of vertical velocities of antihydrogen in GBARDufour, G.;Debu, P.;Lambrecht, A.;Nesvizhevsky, V. V.;Reynaud, S.;Voronin, A. Yu.
doi: 10.1140/epjc/s10052-014-2731-8pmid: N/A
Abstract GBAR is a project aiming at measuring the free-fall acceleration of gravity for antimatter, namely antihydrogen atoms (\(\overline{\mathrm {H}}\)). The precision of this timing experiment depends crucially on the dispersion of initial vertical velocities of the atoms as well as on the reliable control of their distribution. We propose to use a new method for shaping the distribution of the vertical velocities of \(\overline{\mathrm {H}}\), which improves these factors simultaneously. The method is based on quantum reflection of elastically and specularly bouncing \(\overline{\mathrm {H}}\) with small initial vertical velocity on a bottom mirror disk, and absorption of atoms with large initial vertical velocities on a top rough disk. We estimate statistical and systematic uncertainties, and we show that the accuracy for measuring the free fall acceleration \(\overline{g}\) of \(\overline{\mathrm {H}}\) could be pushed below \(10^{-3}\) under realistic experimental conditions.